2025A&A...693A.269B


Query : 2025A&A...693A.269B

2025A&A...693A.269B - Astronomy and Astrophysics, volume 693A269 (2025/1-1)

A BCool survey of stellar magnetic cycles.

BELLOTTI S., PETIT P., JEFFERS S.V., MARSDEN S.C., MORIN J., VIDOTTO A.A., FOLSOM C.P., SEE V. and DO NASCIMENTO J.-D.Jr

Abstract (from CDS):

Context. The magnetic cycle on the Sun consists of two consecutive 11-yr sunspot cycles and exhibits a polarity reversal around sunspot maximum. Although solar dynamo theories have progressively become more sophisticated, the details as to how the dynamo sustains magnetic fields are still the subject of research. Observing the magnetic fields of Sun-like stars can bring useful insights to contextualise the solar dynamo.
Aims. With the long-term spectropolarimetric monitoring of stars, the BCool survey studies the evolution of surface magnetic fields to understand how dynamo-generated processes are influenced by key ingredients, such as mass and rotation. Here, we focus on six Sun-like stars with masses between 1.02 and 1.06 M⊙ and with rotation periods of 3.5-21 d (or 0.3-1.8 in Rossby numbers), a practical sample with which to study magnetic cycles across distinct activity levels.
Methods. We analysed high-resolution spectropolarimetric data collected with ESPaDOnS, Narval, and Neo-Narval between 2007 and 2024 within the BCool programme. We measured longitudinal magnetic field from least-squares deconvolution line profiles and we inspected its long-term behaviour with both a Lomb-Scargle periodogram and a Gaussian process. We then applied Zeeman-Doppler imaging to reconstruct the large-scale magnetic field geometry at the stellar surface for different epochs.
Results. Two of our slow rotators, namely HD 9986 and HD 56124 (Prot ∼ 20 d), exhibit repeating polarity reversals in the radial or toroidal field component on shorter timescales than the Sun (5-6 yr). HD 73350 (Prot ∼ 12 d) has one polarity reversal in the toroidal component and HD 76151 (Prot = 17 d) may have short-term evolution (2.5 yr) modulated by the long-term (16 yr) chromospheric cycle. Our two fast rotators, HD 166435 and HD 175726 (Prot = 3 - 5 d), manifest complex magnetic fields without an evident cyclic evolution.
Conclusions. Our findings indicate the potential dependence of the magnetic cycles' nature on the stellar rotation period. For the two stars with likely cycles, the polarity reversal timescale seems to decrease with a decreasing rotation period or Rossby number. These results represent important observational constraints for dynamo models of solar-like stars.

Abstract Copyright: © The Authors 2025

Journal keyword(s): techniques: polarimetric - stars: activity - stars: magnetic field

Simbad objects: 25

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Number of rows : 25
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 HD 9986 PM* 01 37 40.8790403832 +12 04 42.170345796   7.43 6.76     G2V 135 0
2 HD 19077 * 03 06 41.6409827520 +57 28 15.916115748   9.37 8.21     K1III 7 0
3 * kap01 Cet BY* 03 19 21.6964175772 +03 22 12.714979884 5.71 5.52 4.85 4.27 3.91 G5V 948 0
4 * eps Eri BY* 03 32 55.8444911587 -09 27 29.739493865 5.19 4.61 3.73 3.00 2.54 K2V 2073 1
5 HD 29615 PM* 04 38 43.9420468776 -27 02 01.804814772   9.08 8.47   7.79 G3V 83 0
6 * 111 Tau BY* 05 24 25.4632701888 +17 23 00.726415944   5.52   4.7   F8V 370 0
7 V* AB Dor TT* 05 28 44.8712165880 -65 26 55.199147208 8.259 7.856 6.999 6.496 5.993 K0V 1080 0
8 V* V1385 Ori SB* 06 01 10.5355697568 +19 25 13.572804216   7.54 7.46     A0 18 0
9 HD 56124 PM* 07 17 09.5324832360 +33 05 31.395695892 7.700 7.560   6.5   G0 103 0
10 V* V401 Hya BY* 08 37 50.2937396460 -06 48 24.779911420 7.577 7.394 6.725 6.365 6.029 G5V 197 0
11 * 5 LMi PM* 08 50 32.2228174512 +33 17 06.195898140   6.738 6.210     F7Vs 192 0
12 HD 76151 PM* 08 54 17.9470964696 -05 26 04.054298491 6.89 6.67 6.00     G2V 580 0
13 HD 78366 PM* 09 08 51.0703818408 +33 52 55.986351384   6.53   5.6   G0IV-V 279 0
14 * tau Boo PM* 13 47 15.7381720026 +17 27 24.809555600 5.02 4.98 4.49 4.09 3.85 F7IV-V 1049 1
15 V* EK Dra BY* 14 39 00.2104038120 +64 17 29.979649860   8.243 7.604     G5VFe-0.7CH-1(k) 500 0
16 * ksi Boo A PM* 14 51 23.3884659504 +19 06 01.619801424   5.40 4.675     G7Ve 564 0
17 * 18 Sco PM* 16 15 37.2702755653 -08 22 09.982125430   6.15 5.50     G2Va 671 0
18 HD 166435 PM* 18 09 21.3816898440 +29 57 06.166145376   7.457 6.829     G1IV 203 0
19 * chi Dra SB* 18 21 03.38255 +72 43 58.2518 4.010 4.070 3.580 3.14 2.83 F7V 420 1
20 V* V889 Her BY* 18 34 20.1028767504 +18 41 24.234675864   8.00 7.449   6.720 G2V 151 0
21 HD 175726 PM* 18 56 37.1723923656 +04 15 54.462836664   7.28 6.71     G0V 124 0
22 HD 190771 PM* 20 05 09.7757965056 +38 28 42.555790200   6.82   5.8   G2V 197 0
23 HD 190711 * 20 13 17.2856686248 -74 48 48.804919380   10.14 8.53     M4III 7 0
24 * 61 Cyg A BY* 21 06 53.9395895022 +38 44 57.902349973 7.50 6.39 5.21 4.19 3.54 K5V 1099 0
25 V* HN Peg BY* 21 44 31.3299461136 +14 46 18.983292600       6.16   G0V+ 561 0

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